A tunable mos operational transconductance amplifier which outputs a differential output current in response to a differential input voltage. The amplifier has a tail current source, a first transistor pair, a second transistor pair and a third transistor pair. The sources of the first and second transistor pairs are connected in common to the tail current source. The third transistor pair is connected in cascode to the first transistor pair. The gates of the second transistor pair are connected to drains of the first transistor pair, respectively. The gates of one of the first transistor pair are connected to each other and a tuning voltage is applied to the gates of the one pair. The differential input voltage is applied between the gates of the other of the first transistor pair and the third transistor pair. The differential output current of the amplifier includes at least the differential drain current of the second transistor pair.

Patent
   5578965
Priority
Jun 13 1994
Filed
Jun 07 1995
Issued
Nov 26 1996
Expiry
Jun 07 2015
Assg.orig
Entity
Large
26
2
EXPIRED
1. A tunable mos operational transconductance amplifier which outputs a differential output current in response to a differential input voltage, comprising:
a tail current source;
first and second transistor pairs having commonly connected sources and driven by said tail current source; and
a third transistor pair connected in cascode to said first transistor pair and serving as loads to said first transistor pair;
gates of said second transistor pair being connected to drains of said first transistor pair, respectively.
19. A tunable mos two-quadrant multiplier which outputs a differential output current in response to the product of values of two input voltages, comprising:
first and second transistor pairs having sources grounded commonly; and
a third transistor pair connected in cascode to said first transistor pair and serving as loads to said first transistor pair;
gates of said second transistor pair being individually connected to drains of said first transistor pair;
a differential input voltage being applied as a first input voltage between gates of said third transistor pair, a second input voltage being applied to gates of said first transistor pair which are connected commonly, the differential output current including at least drain currents of said second transistor pair.
20. A tunable mos two-quadrant multiplier which outputs a differential output current in response to the product of values of two input voltages, comprising:
first and second transistor pairs having sources grounded commonly; and
a third transistor pair connected in cascode to said first transistor pair and serving as loads to said first transistor pair;
drains of said second transistor pair being connected not in cross-coupling to drains of said third transistor pair;
gates of said second transistor pair being individually connected to drains of said first transistor pair;
a differential input voltage being applied as a first input voltage between gates of said first transistor pair, a second input voltage being applied to gates of said third transistor pair which are connected commonly, the differential output current including at least drain currents of said second transistor pair.
17. A tunable mos operational transconductance amplifier which outputs a differential output current in response to a differential input voltage, comprising:
a first tail current source;
a second tail current source;
first and second transistor pairs having drains cross-coupled to each other and having sources connected commonly to said first tail current source; and
a differential pair constituted from transistors connected in cascode and connected to said second tail current source;
gates of transistors on upper stage side constituting said differential pair being connected in common to be applied a tuning voltage thereto, sources of said transistors on the upper stage side being connected to the gates of said first transistor pair, respectively, gates of transistors on lower stage side which constitute said differential pair being connected to gates of said second transistor pair, respectively.
2. The tunable mos operational transconductance amplifier according to claim 1, wherein the drains of said second transistor pair and the drains of said third transistor pair are cross-coupled.
3. The tunable mos operational transconductance amplifier according to claim 1, wherein the drains of said second transistor pair and the drains of said third transistor pair are connected in parallel.
4. The tunable mos operational transconductance amplifier according to claim 1, wherein the drain currents of said third transistor pair are not included in the differential output current, and a power source voltage is applied to the drains of said third transistor pair.
5. The tunable mos operational transconductance amplifier according to claim 1, wherein the tuning voltage is applied to the gates of said first transistor pair which are connected to each other, and the differential input voltage is applied between the gates of said third transistor pair.
6. The tunable mos operational transconductance amplifier according to claim 1, wherein the differential input voltage is applied between the gates of said first transistor pair, and the gates of said third transistor pair are connected to each other.
7. The tunable mos operational transconductance amplifier according to claim 6, wherein a voltage from the commonly connected sources of said first and second transistor pairs is coupled as tuning voltage to the gates of said third transistor pair.
8. The tunable mos operational transconductance amplifier according to claim 6, further comprising an operational amplifier for adding a voltage inputted thereto to a voltage from the commonly connected sources of said first and second transistor pairs and outputting a voltage obtained by the addition, an output of said operational amplifier being applied as the tuning voltage to the gates of said third transistor pair.
9. The tunable mos operational transconductance amplifier according to claim 6, further comprising a first auxiliary transistor having a diode connection and connected to a common node of the gates of said third transistor pair, and a second auxiliary transistor interposed between the common sources of said first and second transistor pairs and the common node, the gate of said second auxiliary transistor being connected to the respective gates of said first transistor pair through a pair of resistors.
10. The tunable mos operational transconductance amplifier according to claim 6, further comprising a fourth transistor pair interposed between said first transistor pair and said third transistor pair, each of transistors which constitute said fourth transistor pair having a diode connection, transistors which constitute said second transistor pairs having transconductance parameters different from transconductance parameters of transistors which constitute the other transistor pairs.
11. The tunable mos operational transconductance amplifier according to claim 10, wherein the transconductance parameters of the transistors which constitute said second transistor pair are equal to one half the transconductance parameters of the transistors which constitute the other transistor pairs.
12. The tunable mos operational transconductance amplifier according to claim 10, wherein the transconductance parameters are made different by making a ratio between a width and a length of a gate different between said transistors.
13. The tunable mos operational transconductance amplifier according to claim 6, further comprising a fourth transistor pair interposed between said first transistor pair and said third transistor pair, each of the transistors which constitute said fourth transistor pair having a diode connection, halves of drain currents of the transistors which constitute said second transistor pair relating to the differential output current.
14. The tunable mos operational transconductance amplifier according to claimed in claim 13, wherein a pair of transistors is connected to each of the drains of the transistors which constitute said second transistor pair to divide drain currents of the transistors which constitute said second transistor pair into two.
15. The tunable mos operational transconductance amplifier of claim 1, wherein a tuning voltage is applied to the gates of said first transistor pair, and a differential input voltage is applied between the gates of said third transistor pair, and wherein the differential output current includes at least drain currents of said second transistor pair.
16. The tunable mos operational transconductance amplifier of claim 1, wherein a tuning voltage is applied to the gates of said third transistor pair, and a differential input voltage is applied between the gates of said first transistor pair, and wherein the differential output current includes at least drain currents of said second transistor pair.
18. The tunable mos operational transconductance amplifier according to claim 17, wherein a second differential pair constituted from transistors connected in cascode is added to said differential pair, transistors on lower stage side of each of the differential pairs having a diode connection, the differential input voltage being applied between gates of transistors on upper stage side of said second differential pair, sources of the transistors on the upper stage side of said second differential pair being connected to the gates of said second transistor pair.
21. The tunable mos two-quadrant multiplier according to claim 20, wherein the drains of said second transistor pair and drains of said third transistor pair are connected in parallel.

1. Field of the Invention

This invention relates to a tunable operational transconductance amplifier (OTA) constructed using MOS (metal-oxide-semiconductor) field effect transistors and a two-quadrant multiplier constituted from a circuit similar to the OTA, and more particularly to a tunable OTA and a two-quadrant multiplier constructed on a semiconductor integrated circuit.

2. Description of the Prior Art

A transconductance amplifier outputs a current which increases in proportion to an input voltage, and is a functional element which is essentially required in analog signal processing. Among various transconductance amplifiers, a tunable OTA whose gain increases in proportion to a controlling voltage (tuning voltage) has a high utility value and is employed widely in semiconductor integrated circuits and large scale integrated circuits (LSIs). Further, the tunable OTA can be employed also as a multiplier because it generates an output current which increases in proportion to the product of an input voltage and a controlling voltage.

As one of tunable OTAs, a circuit proposed by Z. Wang and W. Guggenbuhl, in IEEE Journal of Solid-State Circuits, Vol. 25, No. 1, pp.315-317, February 1990 is known. FIG. 1 shows the construction of the MOS OTA by Wang et al. The circuit includes eight MOS transistors M1 to M8 having same characteristics. The sources of MOS transistors M1 to M4 are connected in common to a power source VSS through a constant current source 11 of a current 2ISS. In particular, a quadritail cell is constituted from transistors M1 to M4. Transistors M5 and M7 are connected in series and interposed between another power source VDD and the power source VSS. Similarly, transistors M6 and M8 connected in series are interposed between the power sources VDD and VSS. The voltages of the power sources VDD and VSS are +5 V and -5 V, respectively.

The gates of transistors M1 and M5 are connected in common to an input terminal A. The gates of transistors M2 and M4 are connected commonly to another input terminal B. Further, the gates of transistors M7 and M8 are connected commonly to a further input terminal C for inputting a tuning voltage. The gate of transistor M3 is connected to the source of transistor M5, and the gate of transistor M4 is connected to the source of transistor M6. The drains of transistors M1 and M4 are connected to each other, and the sum of the drain currents of transistors M1 and M2 is represented by I1. Similarly, the drains of the transistors M2 and M3 are connected commonly, and the sum of the drain currents of the transistors M2 and M3 is represented by I2.

In the present OTA, a differential input voltage is applied between the input terminals A and B, and a tuning voltage VB is applied between the input terminal C and the power source VSS. A differential current ΔI between the currents I1 and I2 represents an output value.

The drain current of an MOS transistor operating in saturation is, ignoring a channel length modulation and a body effect, given by ##EQU1## where β is a transconductance parameter and is given by β=μ(COX /2)(W/L). μ is the effective mobility of carriers, COX is the gate oxide film capacitance per unit area, and W and L are the gate width and the gate length, respectively. Further, VTH represents the threshold voltage, and VGSi represents the gate-source voltage of the i-th transistor.

Since the transistors have same characteristics and the equal tuning voltage VB is applied to the gates of transistors M7 and M8, the drain currents of the two transistors M7 and M8 are equal to each other. Where the drain current value is represented by IB, also the drain currents of transistors M5 and M6 are equal to IB. Consequently, both of the gate-to-source voltages VGS5 and VGS6 of the transistors M5 and M6 are equal to the tuning voltage VB. Accordingly, the drain currents ID1 to ID4 of the transistors M1 to M4 are represented as given by the following equations:

ID1 =β(Vi /2+VR -VS -VTH)2( 2)

ID2 =β(-Vi /2+VR -VS -VTH)2( 3)

ID3 =β(Vi /2-VB +VR -VS -VTH)2( 4)

ID4 =β(-Vi /2-VB +VR -VS -VTH)2( 5)

where Vi is the input differential voltage, VR is the midpoint voltage (dc voltage) of the input signal, and VS is the common source voltage.

From the requirement for the tail currents, the following equation stands:

ID1 +ID2 +ID3 +ID4 =Io ( 6)

After all, the differential output current ΔI of the tunable MOS OTA is represented by the following equation: ##EQU2##

As can be seen from equation (7), assuming that the square-law of the input/output characteristic of an MOS field effect transistor stands, the circuit operates linearly and the different output current ΔI increases in proportion to the product of the differential input voltage Vi and the tuning voltage VB within an input voltage range in which none of the MOS transistors in the circuit cuts off. As the differential input voltage Vi becomes higher, the MOS transistors in the circuit begin to enter a cutoff condition and the circuit goes out of linear operation.

FIG. 2 shows the transfer characteristic of the conventional MOS OTA described above using the tuning voltage VB as a parameter based on equation (7). It can be seen from FIG. 2 that, when the input voltage is high, the differential output current ΔI is limited by the tail current. Further, the transconductance characteristic of the conventional MOS OTA is obtained, by differentiating equation (7) by the input voltage Vi, as given by the following equation: ##EQU3##

FIG. 3 shows the transconductance characteristic obtained in this manner using the tuning voltage VB as a parameter.

By the way, in a semiconductor integrated circuit or a large scale integrated circuit, miniaturization of a circuit pattern is proceeding, and as the miniaturization proceeds, also the power source voltage used decreases from the conventional voltage of 5 V to 3.3 V or further to 3 V. Consequently, the necessity for circuits which operate at a low voltage is further increasing. A CMOS process as an LSI manufacturing process is recognized as an optimum process technology, and it is demanded to realize an OTA of the CMOS configuration. Further, for the conventional OTA described above, it is demanded to decrease the number of transistors constituting the circuit or expand the range of the linear operation.

A multiplier can be constructed using a tunable OTA, and as one of MOS multipliers, a circuit is revealed by K. Bult and H. Wallinga in IEEE Journal of Solid-State Circuits, Vol. SC-21, No. 3, pp.430-435, June 1986 is known. K. Bult et al. discloses both of a two-quadrant multiplier and a four-quadrant multiplier. FIG. 4 is a circuit diagram showing an example of the construction of the two-quadrant multiplier by K. Bult et al.

The multiplier includes six MOS transistors M1 to M6 having same characteristics. The sources of transistors M1 to M4 are grounded in common. Transistors M5 and M6 are connected in series to the drains of transistors M1 and M2, respectively. The drains of transistors M3 and M6 are connected to each other, and a combined current of the drain currents of them is represented by IL. Similarly, the drains of transistors M4 and M5 are connected to each other, and the sum of the drain currents of them is represented by IR. Further, input voltages V1 and V1 ' are applied to the gates of transistors M1 and M2, respectively. The input voltages V1 and V1 ' define a differential input voltage. The gates of transistors M5 and M6 are connected to each other, and a second input voltage V2 is applied to them. Further, the gates of transistors M3 and M4 are connected to the drains of transistors M1 and M2, respectively. The two-quadrant multiplier by the K. Bult and H. Wallinga can be regarded as being constructed as a combination of a first voltage-controlled V-I converter constituted from transistors M1, M3 and M5 and a second voltage-controlled converter constituted from transistors M2, M4 and M6.

If it is assumed that the drain current of a MOS transistor operates in accordance with equation (1) given above, drain currents ID1 to ID4 of the transistors are represented as given by the following equations:

ID1 =β(V1 -VTH)2 ( 9)

ID2 =β(V1 '-VTH)2 ( 10)

ID3 =β(V2 -V1 -VTH)2 ( 11)

ID4 =β(V2 -V1 '-VTH)2 ( 12)

Accordingly, the differential output current ΔI is represented as ##EQU4## where V1 =VR1 +Vi /2, V1 '=VR1 -Vi /2, and V2 =VC. Further, VR1 is the reference voltage with respect to the differential input voltage.

Here, since VTH is a fixed value, the conventional MOS two-quadrant multiplier shown in FIG. 4 outputs, ignoring the threshold level VTH, the differential current ΔI which increases in proportion to the product of the differential input voltage Vi and the second input voltage V2.

Also for MOS two-quadrant multipliers, it is demanded to expand the range of linear operation and allow operation at a further decreased voltage.

It is a first object of the present invention to provide an MOS OTA which is superior in linearity and can be realized with a circuit configuration of a comparatively small scale.

It is a second object of the present invention to provide an MOS two-quadrant multiplier which is superior in linearity and allows an input voltage signal to be applied easily.

The first object of the present invention described above is attained by a tunable MOS operational transconductance amplifier which outputs a differential output current in response to a differential input voltage, comprising a tail current source, first and second transistor pairs connected commonly at sources thereof and driven by the tail current source, and a third transistor pair connected in cascode to the first transistor pair and serving as loads to the first transistor pair, gates of the second transistor pair being connected to drains of the first transistor pair, a tuning voltage being applied to gates of one of the first transistor pair and the third transistor pair which are connected commonly while the differential input voltage is applied between the gates of the other of the first transistor pair and the third transistor pair, the differential output current including at least drain currents of the second transistor pair.

The first object of the present invention described above is attained also by a tunable MOS operational transconductance amplifier which outputs a differential output current in response to a differential input voltage, comprising a first tail current source, a second tail current source, first and second transistor pairs having drains cross-coupled to each other and having sources connected commonly to the first tail current source, and a differential pair constituted from transistors connected in cascode and connected to the second tail current source, gates of transistors on upper stage side constituting the differential pair being connected in common to be applied a tuning voltage thereto, sources of the transistors on the upper stage side being connected to the gates of the first transistor pair, respectively, gates of transistors on lower stage side which constitute the differential pair being connected to gates of the second transistor pair, respectively, the differential input voltage being applied between the gates of the second transistor pair.

The second object of the present invention described above is attained by a tunable MOS two-quadrant multiplier which outputs a differential output current in response to the product of values of two input voltages, comprising first and second transistor pairs having sources grounded commonly, and a third transistor pair connected in cascode to the first transistor pair and serving as loads to the first transistor pair, gates of the second transistor pair being individually connected to drains of the first transistor pair, a differential input voltage being applied as a first input voltage between gates of the third transistor pair, a second input voltage being applied to gates of the first transistor pair which are connected commonly, the differential output current including at least drain currents of the second transistor pair.

The second object of the present invention described above is attained also by a tunable MOS two-quadrant multiplier which outputs a differential output current in response to the product of values of two input voltages, comprising first and second transistor pairs having sources grounded commonly, and a third transistor pair connected in cascode to the first transistor pair and serving as loads to the first transistor pair, drains of the second transistor pair being connected not in cross-coupling to drains of the third transistor pair, gates of the second transistor pair being individually connected to drains of the first transistor pair, a differential input voltage being applied as a first input voltage between gates of the first transistor pair, a second input voltage being applied to gates of the third transistor pair which are connected commonly, the differential output current including at least drain currents of the second transistor pair.

The above and other objects, features, and advantages of the present invention will become apparent from the following description when taken in conjunction with the accompanying drawings which illustrate preferred embodiments of the present invention by way of example.

FIG. 1 is a circuit diagram of the construction of a conventional tunable MOS OTA;

FIG. 2 is a graph showing the transfer characteristic of the conventional OTA shown in FIG. 1;

FIG. 3 is a graph showing the transconductance characteristic of the conventional OTA shown FIG. 1;

FIG. 4 is a circuit diagram showing the construction of a conventional MOS two-quadrant multiplier;

FIG. 5 is a circuit diagram showing the construction of an example of an MOS OTA according to a first embodiment of the present invention;

FIGS. 6, 7, 8, 9 and 10 are circuit diagrams individually showing different examples of the MOS OTA according to the first embodiment of the present invention;

FIG. 11 is a circuit diagram showing the construction of an MOS OTA according to a second embodiment of the present invention;

FIG. 12 is a circuit diagram showing the construction of an MOS OTA according to a third embodiment of the present invention;

FIG. 13 is a circuit diagram showing an example of the construction of an MOS OTA according to a fourth embodiment of the present invention;

FIG. 14 is a circuit diagram showing another example of the construction of the MOS OTA according to the fourth embodiment of the present invention;

FIG. 15 is a circuit diagram showing the construction of an MOS OTA according to a fifth embodiment of the present invention;

FIG. 16 is a circuit diagram showing the construction of an MOS OTA according to a sixth embodiment of the present invention;

FIG. 17 is a circuit diagram showing an example of the construction of an MOS two-quadrant multiplier according to a seventh embodiment of the present invention; and

FIGS. 18 to 21 are circuit diagrams individually showing different examples of the construction of the MOS two-quadrant multiplier according to the seventh embodiment of the present invention.

PAC <<First Embodiment>>

The MOS OTA of the first embodiment of the present invention includes six MOS transistors M1 to M6 as shown in FIG. 5. The sources of the four transistors M1 to M4 are connected to each other and grounded through a constant current source 21 whose current value is represented by Io. Further, transistors M5 and M6 are connected as loads to the drains of transistors M1 and M2, respectively. The gates of transistors M3 and M4 are connected to the drains of transistors M1 and M2, respectively. Transistors M1 to M4 constitute a quadritail cell since they share a single tail current Io. However, since transistors M5 and M6 are connected in cascode to transistors M1 and M2, the circuit of the type just described is hereinafter referred to as cascode quadritail cell.

The gates of transistors M1 and M2 are connected to each other, and a tuning voltage VC is applied to them. A differential input voltage Vi is applied between the gates of transistors M5 and M6. Further, the drains of transistors M5 and M6 are connected in common to a power source voltage VDD. Here, drain currents ID3 and ID4 of transistors M3 and M4 are represented as currents IL and IR, respectively.

Where the gate-source voltage of the i-th transistor is represented by VGSi and the drain current of the i-th transistor is represented by IDi, since ID1 =ID2 and VGS1 =VGS2 =VGS5 =VGS6 stand, drain currents ID1 to ID4 of transistors M1 to M4 are represented as given by the following equations:

ID1 =ID2 =β(VC -VS -VTH)2(14)

ID3 =β(Vi /2+VR -VC -VTH)2(15)

ID4 =β(-Vi /2+VR -VC -VTH)2(16)

where β is the transconductance parameter of the transistor, VR is the reference voltage corresponding to the midpoint voltage of the differential input voltage, and VTH is the threshold voltage.

Meanwhile, from the requirement for the tail currents, the following equation stands:

ID1 +ID2 +ID3 +ID4 =Io (17)

Accordingly, the differential input current ΔI is represented as ##EQU5## The common source voltage VS relies upon the differential input voltage Vi and is represented as ##EQU6## However, the differential output current ΔI does not rely upon the common source voltage VS as seen from equation (18), and after all, the present circuit outputs the differential output current ΔI which increases in proportion to the input voltage Vi. In short, the present circuit operates linearly.

In the MOS OTA shown in FIG. 5 and described above, the difference between drain currents ID3 and ID4 of transistors M3 and M4 in pair is obtained as the differential output current ΔI. However, the differential output current ΔI may be obtained by various other methods from the drain currents ID1 to ID4 of the quadritail cell. In the MOS OTA of Example 2 shown in FIG. 6, the upper side transistor of the cascoded transistor pairs and the other transistor pair constituting the quadritail cell are connected in parallel, and the drains of transistors M5 and M6 are connected to the drains of transistors M3 and M4, respectively. Accordingly, the output differential current ΔI of the present MOS OTA is represented as given below: ##EQU7##

Meanwhile, in the MOS OTA of Example 3 shown in FIG. 7, the two transistor pairs constituting the quadritail cell are cross-coupled, and the drains of transistors M5 and M6 are connected to the drains of transistors M4 and M3, respectively. Accordingly, the output differential current ΔI of the present MOS OTA is represented as given below: ##EQU8##

As apparently seen from equations (20) and (21), both of the MOS OTAs shown in FIGS. 6 and 7 have a same input/output characteristic as that of the MOS OTA shown in FIG. 5 and operate linearly.

While the MOS OTAs shown in FIGS. 5, 6 and 7 are constructed such that the differential input voltage Vi is applied to that one of the two transistor pairs connected in cascode which is remote from the tail current source 21, it is possible to otherwise employ another construction wherein the differential input voltage Vi is inputted to that transistor pair closer to the tail current source 21. While the MOS OTA of Example 4 shown in FIG. 8 has a similar construction to the OTA shown in FIG. 5, it is different in construction in that the differential input voltage Vi is applied between the gates of transistors M1 and M2 and the tuning voltage VC is applied to the gates of transistors M5 and M6 which are connected to each other.

Since VGS1 =VGS5, VGS2 =VGS6, ID1 =ID5 and ID2 =ID6 stand with the construction just described, drain currents ID1 to ID4 of transistors M1 to M4 are represented as given below:

ID1 =β(Vi /2+VR -VS -VTH)2(22)

ID2 =β(-Vi /2+VR -VS -VTH)2(23)

ID3 =β(VC -Vi /2-VR -VTH)2(24)

ID4 =β(VC +Vi /2-VR -VTH)2(25)

Since equation (17) described above stands from the requirements for the tail current Io, the differential output current ΔI is given by: ##EQU9##

In the present circuit, the common source current VS relies upon the differential input voltage Vi and is represented as given by the following equation: ##EQU10##

Since the common source voltage VS does not appear in equation (26), the present circuit operates linearly.

The MOS OTA of Example 5 shown in FIG. 9 employs a balanced-cascoded quadritail cell and is different in construction from the OTA shown in FIG. 6 in that the differential input voltage Vi is applied between the gates of transistors M1 and M2 and the tuning voltage VC is applied to the gates of transistors M5 and M6 which are connected to each other. In the present circuit, equations (22) to (25) given above stand with regard to drain currents ID1 to ID4 of transistors M1 to M4, and further, equations (17) and (27) stand. Consequently, the differential output current ΔI is represented as given below: ##EQU11##

In the present circuit, the common source voltage VS relies upon the differential input voltage Vi as seen from equation (27), and the differential output current ΔI includes a term of the common source voltage VS as seen from equation (28). Accordingly, the term of the common source voltage VS is a non-linear term of the differential output current ΔI and deteriorates the linearity of the output of the circuit.

The MOS OTA of Example 6 shown in FIG. 10 employs an unbalanced-cascoded quadritail cell and is different in construction from the OTA shown in FIG. 7 in that the differential input voltage Vi is applied between the gates of transistors M1 and M2 and the tuning voltage VC is applied to the gates of transistors M5 and M6 which are connected to each other. In the present circuit, equations (22) to (25) stand with regard to drain currents ID1 to ID4 of the transistors M1 to M4, and further, equations (17) and (27) stand. Consequently, the differential output current ΔI is represented as given below: ##EQU12##

Also in the present circuit, the differential output current ΔI includes a term of the common source voltage VS similarly to the circuit shown in FIG. 9. Accordingly, this term is a non-linear term of the differential output current ΔI and deteriorates the linearity of the output of the circuit.

In the MOS OTAs of the first embodiment shown in FIGS. 5 to 10, a floating input is realized by driving the transistors with a constant current using a cascoded quadritail cell. Further, linear operation is realized with the MOS OTAs of Examples 1 to 4 shown in FIGS. 5 to 8, respectively. Meanwhile, with the MOS OTAs of Examples 5 and 6 shown in FIGS. 9 and 10, linear operation is not realized, and the linearity with respect to the tuning voltage is sacrificed.

As described above, with the MOS OTA shown in FIG. 9, linear operation cannot be realized since the differential output current ΔI is varied also by the common source voltage VS. However, as apparently seen from equation (28), by applying a tuning voltage to a balanced-cascoded quadritail cell with reference to the common source voltage VS, the term of the common source voltage VS can be eliminated from the equation representing the differential output current ΔI, and linear operation can be realized. In the MOS OTA of the second embodiment of the present invention shown in FIG. 11, the level of the control voltage VB inputted from the outside is shifted using an operational amplifier 30 so that a tuning voltage VC with reference to the common source voltage VS may be applied to the cascode quadritail cell. In particular, two resistors R having an equal resistance value and connected in series are interposed between the common gates of transistors M5 and M6 and the common sources of transistors M1 to M4, and the tuning voltage VB is inputted to the (+) input terminal of the operational amplifier 30 while the (-) input terminal of the operational amplifier 30 is connected to the midpoint of the two resistors R. Further, the output terminal of the operational amplifier 30 is connected commonly to the gates of transistors M5 and M6.

The MOS OTA of the third embodiment of the present invention shown in FIG. 12 is a modification to the MOS OTA shown in FIG. 5 in that it additionally includes two MOS transistors M7 and M8 and two resistors R having an equal resistance value so that the tuning voltage VC may be applied to the cascode quadritail cell with reference to the common source voltage VS. Transistors M7 and M8 are connected in series, and the source of transistor M7 is connected to the sources of transistors M1 to M4 while the drain and the gate of transistor M8 are connected to each other and the tuning voltage VB is applied to the drain and the gate of the transistor M8. The drain of transistor M7 is connected to the gates of the transistors M5 and M6. The two resistors R are interposed in series between the gate of transistor M1 and the gate of transistor M2, and the midpoint of the series connection is connected to the gate of transistor M7.

Since also transistor M7 shares the tail current source 11, the present circuit is accurately called balanced-cascoded quint-tail cell. The tuning voltage VC as measured from the grounding point, that is, the gate voltage of transistors M5 and M6 is given by

VC =VB -VR +VS -VTH (30)

By substituting equation (30) into equation (28), it can be recognized that the differential output current ΔI in the present circuit does not rely upon the common source voltage VS, and linear operation is realized.

An MOS OTA (refer to FIG. 10) which employs an unbalanced-cascoded quadritail cell can be constructed as a circuit which does not rely upon the common source voltage VS by connecting transistors in cascode in three stages and varying the transistor sizes of them to vary the transconductance parameters. This circuit operates linearly. FIG. 13 shows an example of the circuit of the type just described. The circuit shown in FIG. 13 is a modification to the circuit shown in FIG. 10 in that an additional transistor M7 is interposed between transistors M1 and M5 and another additional transistor M8 is interposed between transistors M2 and M6, and while each of transistors M1, M2, M5, M6, M7 and M8 have a same transconductance parameter β, the transistors M3 and M4 have another transconductance parameter Kβ. The drain and the gate of transistor M7 are connected to each other, and similarly, the drain and the gate of transistor M8 are connected to each other. When K=1/2, the differential output current ΔI of the present unbalanced-double-cascoded quadritail cell is given by

ΔI=4βVi (VC -VR -2VTH) (31)

Particularly, in order to achieve K=1/2, the ratio between the width W and the length L of the gates of transistors M3 and M4 should be equal to one half the W/L ratio of the other transistors M1, M2, M5 and M6.

Or, in order to construct a circuit similar to that shown in FIG. 13 using transistors of an equal size, that is, using transistors having an equal transconductance parameter β, the circuit should be so constructed that currents equal to one half the currents flowing individually through the transistors M3 and M4 contribute to the differential output current ΔI. In particular, as shown in FIG. 14, transistors M9 and M10 are connected to the drain of transistor M3; the drain of transistor M9 is connected to the drain of transistor M8; and the power source voltage is supplied to the drain of transistor M10. Further, the gates of transistors M9 and M10 are connected in common to the drain of the transistor M9. Similarly, transistors M11 and M12 are connected to the drain of transistor M4, and the gates of transistors M11 and M12 are connected to the drain of transistor M11. Further, the drain of transistor M11 is connected to the drain of transistor M7, and the power source voltage is supplied to the drain of transistor M12. Here, the transconductance parameters of transistors M3 and M4 are equal to that of the other transistors. By the construction described above, the drain currents flowing through transistors M9 and M11 are equal to one half the currents flowing through transistors M3 and M4, respectively, and the circuit exhibits an input/output characteristic equivalent to that of the circuit shown in FIG. 13.

If it is intended to reduce a transconductance parameter to one half using a single transistor, then a quadruple area is required. Accordingly, with the circuit shown in FIG. 13, an area equal to a total area of 14 transistors whose transconductance parameter is β is required. In contrast, the circuit shown in FIG. 14 requires 12 transistors whose transconductance parameter is β. Anyway, since those circuits include a cascode connection of transistors in three stages, it is difficult to lower the power source voltage to those circuits.

The MOS OTA of the present invention includes a circuit of the type wherein an offset generator as an inputting circuit is added to the quadritail cell circuit by Wang et al. shown in FIG. 1. The offset generator may employ a cascode differential pair wherein transistors are connected in cascode or a cascode quadritail cell which includes a voltage divider.

In the MOS OTA shown in FIG. 15, an MOS voltage adder constituted from a cascode differential pair is employed as an inputting circuit, and a tunable offset circuit is realized. The sources of four transistors M1 to M4 are connected to each other and are grounded via a tail current source 22 of a constant current Io. The drains of transistors M1 and M4 are connected to each other, and the sum of drain currents ID1 and ID4 of transistors M1 and M4 is represented by a current IR. Similarly, the drains of transistors M2 and M3 are connected to each other, and the sum of drain currents ID2 and ID3 is represented by a current IL. A pair of transistors M5 and M6 whose sources are connected to each other and which are driven by a second tail current source 23 represented by another constant current Ib are provided, and transistors M7 and M8 are connected to the drains of transistors M5 and M6, respectively. A power source voltage is supplied to the drains of transistors M7 and M8, and the gates of transistors M7 and M8 are connected to each other and a tuning voltage VC is applied to the gates of transistors M7 and M8. The gates of transistors M3 and M4 are connected to the drains of transistors M5 and M6, respectively. The gate of transistor M1 and the gate of transistor M5 are connected to each other, and the gate of transistor M2 and the gate of transistor M6 are connected to each other. A differential input voltage Vi is applied between the gate of transistor M5 and the gate of transistor M6.

In the present circuit, a cascode differential pair is constituted from transistors M5 to M8, and the circuit acts as a voltage adder.

In the MOS OTA shown in FIG. 16, a cascode quadritail cell which includes a voltage divider is employed as an inputting circuit, and a tunable offset circuit is realized. In particular, a quadritail cell is constituted from transistors M1 to M4, and a cascode quadritail cell is constituted from transistors M5 to M12. The sources of transistors M1 to M4 are connected in common to a first tail current source 22 of a constant current Io, and the sources of transistors M5 to M8 are connected in common to another second tail current source 23 of a constant current Ib. The drains of transistors M1 and M4 are connected to each other, and the sum of drain currents ID1 and ID4 of transistors M1 and M4 is represented by a current IR. Similarly, the drains of transistors M2 and M3 are connected to each other, and the sum of drain currents ID2 and ID3 of transistors M2 and M3 is represented by a current IL.

Transistors M9 to M12 are connected to the drains of transistors M5 to M8, respectively, and a power source voltage is supplied to the drains of transistors M9 to M12. The gates of transistors M1, M5 and M6 are connected in common to the drain of transistor M5, and the gates of transistors M2, M7 and M8 are connected in common to the drain of transistor M8. In particular, a first current mirror circuit is constituted from transistors M5 and M6, and a second current mirror circuit is constituted from transistors M7 and M8. The gates of transistors M3 and M4 are connected to the drains of transistors M6 and M7, respectively. Further, the gates of transistors M11 and M12 are connected to each other, and the tuning voltage VC is applied to the gates of transistors M11 and M12 while the differential input voltage Vi is applied between the gate of transistor M9 and the gate of transistor M12.

The tunable MOS OTAs of the embodiments described above can be used also as MOS two-quadrant multipliers. Examples of the construction of the MOS two-quadrant multiplier according to the present invention are described below.

The MOS two-quadrant multiplier shown in FIG. 17 is equivalent to the construction of the MOS OTA shown in FIG. 5 from which the tail current source is removed. The sources of transistors M1 to M4 are grounded directly, and the gates of transistors M1 and M2 are connected to each other and a first input voltage V1 is applied to the gates of transistors M1 and M2. Meanwhile, voltages V2 and V2 ' are inputted as second voltages to the gates of transistors M5 and M6, respectively. The voltages V2 and V2 ' define a differential input voltage.

Since VGS1 =VGS2 =VGS5 =VGS6 =V1 and ID1 =ID2 stand with the present circuit, the drain currents ID1 to ID4 of transistors M1 to M4 are represented as given by the following equations:

ID1 =ID2 =β(V1 -VTH)2 (32)

ID3 =β(V2 -V1 -VTH)2 (33)

ID4 =β(V2 '-V1 '-VTH)2 (34)

Accordingly, the differential output current ΔI is given by ##EQU13## where V1 =VC, V2 =VR1 -Vi /2 and V2 '=VR1 +Vi/ 2, and VR1 is the midpoint voltage of the differential potential Vi (=V2 -V2 '). Accordingly, the present two-quadrant multiplier operates linearly.

The MOS two-quadrant multipliers of Examples 2 and 3 shown in FIGS. 18 and 19 are modifications to the MOS OTAs shown in FIGS. 6 and 7, respectively, in that the tail current source is removed and the sources of transistors M1 to M4 are grounded directly. Similarly to Example 1 described above, a first input voltage V1 and second input voltages V2 and V2 ' as a differential input voltage are applied to the present MOS two-quadrant multipliers. Also with the present circuits, drain currents ID1 to ID4 of transistors M1 to M4 are represented by equations (32) to (34).

Accordingly, the differential output current ΔI of the circuit of FIG. 18 is represented as given by ##EQU14## while the differential output current ΔI of the circuit of FIG. 19 is represented as given by ##EQU15## After all, both of the circuits of FIGS. 18 and 19 have a same input/output characteristic as that of the circuit of FIG. 17, and operate linearly.

The differential output type MOS two-quadrant multiplier of Example 4 shown in FIG. 20 is a modification in construction to the MOS OTA shown in FIG. 8 in that the tail current source is removed. The sources of transistors M1 to M4 are grounded directly, and input voltages V1 and V1 ' are applied to the gates of transistors M1 and M2, respectively. Further, the gates of transistors M5 and M6 are connected to each other, and a second input voltage V2 is applied to the gates of transistors M5 and M6. The input voltages V1 and V1 ' constitute a differential input voltage.

In the present circuit, since VGS1 =VGS5 =V1 and VGS2 =VGS6 =V1 ', the drain currents ID1 to ID4 of transistors M1 to M4 are represented in the following manner:

ID1 =β(V1 -VTH)2 (38)

ID2 =β(V1 '-VTH)2 (39)

ID3 =β(V2 -V1 -VTH)2 (40)

ID4 =β(V2 -V1 '-VTH)2 (41)

Accordingly, the differential output current ΔI is represented as ##EQU16## where V1 =VR1 +Vi /2, V1 '=VR1 -Vi /2 and V2 =VC.

The balanced MOS two-quadrant multiplier of Example 5 shown in FIG. 21 is a modification to the MOS OTA shown in FIG. 9 in that the tail current source is removed. The sources of the transistors M1 to M4 are grounded directly, and input voltages V1 and V1 ' are applied to the gates of transistors M1 and M2, respectively. Further, the gates of transistors M5 and M6 are connected to each other, and a second input voltage V2 is applied to the gates of transistors M5 and M6. The input voltages V1 and V1 ' define a differential input voltage. Since drain currents ID1 to ID4 of transistors M1 to M4 are represented as given by equations (38) to (41) above, the differential output current of the present circuit is represented as ##EQU17## Accordingly, the present multiplier has a circuit characteristic which depends upon a voltage applied thereto without being influenced by the threshold voltage VTH. In other words, the present multiplier operates equivalently to a differential pair having floating inputs. Further, the power source voltage can be made lower as the sources of the transistors are grounded.

The unbalanced two-quadrant multiplier (refer to FIG. 4) proposed by K. Bult and H. Wallinga can be regarded as a circuit which includes a combination of two sets of voltage-controlled V-I converter circuits. For a circuit of the type just mentioned, two methods for applying an input voltage and three methods of obtaining an output differential current are available similarly as described hereinabove in connection with the first embodiment, and totaling six different circuits can be provided by combinations of them. While K. Bult and H. Wallinga discloses only one of the six possible circuits, the remaining five circuits are disclosed in Examples 1 to 5 described above. It is to be noted that the differential output current ΔI of the circuit by K. Bult and H. Wallinga includes a term of the threshold voltage VTH as seen from equation (13). This similarly applies to the circuits shown in FIGS. 17 to 20.

Although certain preferred embodiments of the present invention have been shown and described in detail, it should be understood that various changes and modifications may be made therein without departing from the scope of the appended claims.

Kimura, Katsuji

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